Large Signal ModelReading edition

94. A nonlinear observable state with a curved moment domain

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94. A nonlinear observable state with a curved moment domain

For \(u\in[-1,1]\), put

\[ v(u)=(1,u,u^2)^{\mathsf T}, \qquad L_2(u)=\frac{3u^2-1}{2}. \]

The normalized states are moments of a scalar signal:

\[ K=\{(1,x,y):x^2\leq y\leq1\}. \]

Their cone has the finite curved description

\[ C=\left\{(m,x,y): \begin{pmatrix}m&x\\x&y\end{pmatrix}\succeq0, \quad m-y\geq0\right\}, \qquad\lambda=(1,0,0). \]

Assume that the declared probability measure \(\mu\) on \([-1,1]\) has moments zero at orders one and three, \(1/3\) at order two and \(1/5\) at order four. Define a two-parameter degree-four operator density

\[ \boxed{ B_{a,b}(u)=v(u)\,(1,au,bL_2(u)). } \]

Here \(a,b\) are parameters, not action labels. This example is autonomous. Its dependence on the observed signal is nonlinear because the state includes its square.

Proposition 83: Structured curved-domain certificate

The set \(K\) is the convex hull of all \(v(u)\). If \(|a|+|b|\leq1-\rho\) for \(0\leq\rho\leq1\), then \(B_{a,b}(u)\) preserves \(C\) and has exact integrated mass. On a normalized state, its density is

\[ p_{a,b}(u\mid x,y)=1+a x u+b yL_2(u)\geq\rho. \]

Every positive-density posterior is exactly \(v(u)\). In particular, starting from \(v(s)\) produces the observable Markov law

\[ p_{a,b}(u\mid s)=1+a s u+b s^2L_2(u). \]

Its next conditional moments satisfy

\[ \boxed{ \mathbb E[U_t\mid U_{t-1}=s]=\frac a3s, \qquad \mathbb E[L_2(U_t)\mid U_{t-1}=s]=\frac b5s^2. } \]

Proof

Every distribution on \([-1,1]\) has \(x^2\leq y\leq1\). Conversely, fix \(|x|<1\). A point mass at \(x\) gives \((x,x^2)\), while the endpoint mixture with mean \(x\) gives \((x,1)\). Their convex combinations give every intermediate \(y\). The cases \(x=\pm1\) are immediate. Homogenizing yields the matrix and scalar inequalities, which also force the only mass-zero cone element to be zero.

On \(K\), \(|x|\leq1\), \(0\leq y\leq1\), \(|u|\leq1\) and \(|L_2(u)|\leq1\). Thus the density is at least \(1-|a|-|b|\). Each operator output is that nonnegative scalar times \(v(u)\), so lies in \(C\). The first and second reference moments imply \(\lambda\int B_{a,b}(u)\,\mu(du)=\lambda\). Normalization cancels the scalar density, yielding \(v(u)\). Symmetry through order three gives \(\int uL_2(u)d\mu=0\). The second and fourth moments give \(\int L_2(u)^2d\mu=1/5\). Integrating \(u\) and \(L_2\) against the density proves the last two formulas. \(\square\)

The posterior ray lies on a curved boundary. Arbitrary perturbations of its output coordinates can destroy validity, as in Proposition 72. Parameter uncertainty inside the declared family behaves differently: it changes the likelihood but not the posterior ray. A certified rectangle in \((a,b)\) can therefore be robust even though a free matrix-entry ball has no positive validity radius.

This is an example of uncertainty that preserves the model's algebraic structure. It is not a claim that every real system obeys the two-parameter family. The feature dictionary \(1,u,u^2\), its geometry, the reference measure and the parameter model are declared inputs to learning.

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